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Page 3 - Interferometers

NSLI-543-2 N-Slit Laser Interferometer
Interferometric Optics
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NSLI-543-2 N-Slit Laser Interferometer
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Based on multiple-prism beam expansion and digital detection the N-slit interferometer allows for the rapid interferometric characterization of transmission optical surfaces in general. A significant advance over traditional point-by-point incoherent microdensitometers and point-by-point incoherent microscopes.

Specifications
Interferometer Configuration: Not Specified
Light Source: 543nm
Output Polarization: Not Specified
RMS Repeatability: Not Specified
RMS Precision: Not Specified
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NSLI-543-1 N-Slit Laser Interferometer
Interferometric Optics
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NSLI-543-1 N-Slit Laser Interferometer
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Based on multiple-prism beam expansion and digital detection the N-slit interferometer allows for the rapid interferometric characterization of transmission optical surfaces in general. A significant advance over traditional point-by-point incoherent microdensitometers and point-by-point incoherent microscopes. 

Specifications
Interferometer Configuration: Not Specified
Light Source: 543nm
Output Polarization: Not Specified
RMS Repeatability: Not Specified
RMS Precision: Not Specified
Data Sheet
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GEMINI Ultra-Stable Interferometer
Nireos
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GEMINI Ultra-Stable Interferometer
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GEMINI is a novel and compact interferometer that can guarantee very high robustness and stability between the two generated replicas of light.  

Specifications
Interferometer Configuration: Not Specified
Light Source: White Light
Output Polarization: Not Specified
RMS Repeatability: Not Specified
RMS Precision: Not Specified
Data Sheet
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GEMINI-2D
Nireos
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GEMINI-2D
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GEMINI-2D Interferometer is the advanced model of the GEMINI, specially designed to: keep constant the dispersion during the scan of the relative delay between the two generated replicas of light keep fixed the absolute arrival time of one of the two replicas (with attosecond stability) The capability of ...

Specifications
Interferometer Configuration: Not Specified
Light Source: White Light
Output Polarization: Not Specified
RMS Repeatability: Not Specified
RMS Precision: Not Specified
Data Sheet
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PicoScale sensor head type L01
SmarAct
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PicoScale sensor head type L01
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The L01 is a sensor head for the PICOSCALE laser interferometer. The target beam is focused along only one axis with a cylinder lens so that a line focus is generated. This way, the sensor head has a relatively large angular working range along the focused axis while having a large diameter along the orthogonal axis. Typically, these ...

Specifications
Interferometer Configuration: Not Specified
Light Source: 1550nm
Output Polarization: Linear
RMS Repeatability: Not Specified
RMS Precision: Not Specified
Data Sheet
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PicoScale Sensor Head Type F01
SmarAct
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PicoScale Sensor Head Type F01
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The F01 is a sensor head type with focused probe beam. This allows to measure displacements of small targets. Furthermore, the sensor heads provide high angular tolerances. After pre-collimation, an integrated beam splitter splits the light into a reference and probe beam as shown in Figure 1. The reference beam is reflected off the ...

Specifications
Interferometer Configuration: Not Specified
Light Source: 1550nm
Output Polarization: Linear
RMS Repeatability: Not Specified
RMS Precision: Not Specified
Data Sheet
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PicoScale Sensor Head Type C03
SmarAct
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PicoScale Sensor Head Type C03
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The C03 is a sensor head type optimized for moderate working distances and using retro-reflectors as target. The probe beam is enlarged so that its divergence is reduced and more optical power can be collected after reflection at the target mirror. The C03 sensor head type is based on the standard sensor head type C01, including the ...

Specifications
Interferometer Configuration: Not Specified
Light Source: 1550nm
Output Polarization: Linear
RMS Repeatability: Not Specified
RMS Precision: Not Specified
Data Sheet
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PicoScale Sensor Head Type C01
SmarAct
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PicoScale Sensor Head Type C01
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The C01 is the standard sensor head type for the PICOSCALE Interferometer. Due to its collimated output beam, the compact form factor and the various customization options, it is appropriate for most common applications. Each sensor head (see figure 1) is based on two main components: the lens system, collimating the fiber output ...

Specifications
Interferometer Configuration: Not Specified
Light Source: 1550nm
Output Polarization: Linear
RMS Repeatability: Not Specified
RMS Precision: Not Specified
Data Sheet
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µPhase® UNIVERSAL - Horizontal Setup For All Kinds of Interferometric Measurements
TRIOPTICS GmbH
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µPhase® UNIVERSAL - Horizontal Setup For All Kinds of Interferometric Measurements
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Optimized for measurements in R&D, the μPhase® UNIVERSAL is the most flexible instrument of the μPhase® product line. The horizontal design enables the measurement of a large variety of lenses and components differing in size, radius and material.

Specifications
Interferometer Configuration: Twyman–Green Interferometer
Light Source: 632 nm or 633nm, 355nm, 532nm, 780nm, 1053nm, 1064nm
Output Polarization: Random
RMS Repeatability: <0.01 waves
RMS Precision: <0.01 waves
Data Sheet
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µPhase® 1000 Flexible Interferometer Sensor
TRIOPTICS GmbH
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µPhase® 1000 Flexible Interferometer Sensor
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These highly integrated phase-shifting Twyman-Green interferometer sensors meet the toughest demands for modern quality management. In combination with the μShape™ measuring and analysis software these high-performance precision measuring instruments provide information about the specimen\'s surface deviation or wave front ...

Specifications
Interferometer Configuration: Twyman–Green Interferometer
Light Source: 632 nm or 633nm
Output Polarization: Random
RMS Repeatability: <0.01 waves
RMS Precision: <0.01 waves
Data Sheet
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µPhase® 500 Flexible Interferometer Sensor
TRIOPTICS GmbH
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µPhase® 500 Flexible Interferometer Sensor
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These highly integrated phase-shifting Twyman-Green interferometer sensors meet the toughest demands for modern quality management. In combination with the µShapeTM measuring and analysis software these high-performance precision measuring instruments provide information about the specimen\'s surface, wavefront or test ...

Specifications
Interferometer Configuration: Twyman–Green Interferometer
Light Source: 632 nm or 633nm
Output Polarization: Random
RMS Repeatability: <0.01 waves
RMS Precision: <0.01 waves
Data Sheet
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AccuFiz Compact Fizeau Laser Interferometers
4D Technology Corporation
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AccuFiz Compact Fizeau Laser Interferometers
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AccuFiz Fizeau interferometers offer an unmatched combination of performance, quality and value, for accurate, repeatable measurement of surface shape and transmitted wavefront quality. AccuFiz laser interferometers are extremely easy to use in confined lab spaces. The compact, lightweight design is extremely rigid for maximum ...

Specifications
Interferometer Configuration: Twyman–Green Interferometer
Light Source: 632 nm or 633nm, 355nm, 532nm, 1053nm, 1064nm, 1550nm, 10.6um
Output Polarization: Circular
RMS Repeatability: <0.00005 waves
RMS Precision: <0.0005 waves
Data Sheet
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PhaseCam Twyman-Green Laser Interferometers
4D Technology Corporation
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PhaseCam Twyman-Green Laser Interferometers
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Twyman-Green configuration interferometers offer several important advantages over more traditional Fizeau instruments: Vibration-insensitive measurement enables use in challenging environments such as cryo-vac testing or over long measurement paths. The design can be extremely compact, enabling use in tight spaces, or in ...

Specifications
Interferometer Configuration: Twyman–Green Interferometer
Light Source: 632 nm or 633nm, 355nm, 532nm, 1053nm, 1064nm, 1550nm, 10.6um
Output Polarization: Circular
RMS Repeatability: <0.001 waves
RMS Precision: <0.002 waves
Data Sheet
Inquire Price